Optical waveform shaper
a waveform and optical technology, applied in optics, instruments, electromagnetic transmission, etc., can solve the problems of reducing the s/n ratio, the receiver cannot demodulate/decode the received signal correctly, and the s/n ratio cannot be improved sufficiently, so as to achieve constant output optical power, improve noise reduction characteristics, and remove noise
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embodiment 1
[0179]The configuration of the optical waveform shaper is the first configuration shown in FIG. 3 or the second configuration shown in FIG. 8A. Specifically, the optical waveform shaper adopts the configuration in which the interferometers 10 and 20 are connected in series, and one of the interferometers has a positive transfer function and the other has a negative transfer function. Also, the following parameters are given.[0180]The γ value of the highly nonlinear optical fibers 12 and 22: 25.0 (1 / (W·km))[0181]The wavelength dispersion of the highly nonlinear optical fibers 12 and 22: −0.5 (ps / nm / km)[0182]The wavelength dispersion slope of the highly nonlinear optical fibers 12 and 22: 0.08 (ps / nm^2 / km)[0183]The γ value of the low nonlinearity optical fibers 13 and 23: 1.3 (1 / (W·km))[0184]The wavelength dispersion of the low nonlinearity optical fibers 13 and 23: −0.5 (ps / nm / km)[0185]The wavelength dispersion slope of the low nonlinearity optical fibers 13 and 23: 0.08 (ps / nm^2 / km)...
embodiment 1-1
[0186]Configuration: The first configuration of FIG. 3[0187]The fiber length in the interferometer 10: 1.0 km[0188]The fiber length in the interferometer 20: 1.0˜10.0 km[0189]Synthesized transfer function: see FIG. 24
[0190]In FIG. 24, a function A represents the transfer function when the fiber length in the interferometer 20 is 1 km. Although the function A seems to have the best characteristics, it has substantially the same transfer function as that of one interferometer (the interferometer 10 in this case). That is to say, it is shown that connecting the interferometer 20 in the subsequent stage does not improve the synthesized transfer function when the fiber length of the interferometer 10 is short.
[0191]Here, a favorable transfer function refers to a function, which meets the following requirements, as explained with reference to FIG. 7.[0192](1) The width of the flat space region FWs is not zero, but has a certain width. When this requirement is satisfied, “0” is obtained as...
embodiment 1-2
[0194]Configuration: The second configuration of FIG. 8A[0195]The fiber length in the interferometer 10: 2.0 km[0196]The fiber length in the interferometer 20: 1.0˜10.0 km[0197]Synthesized transfer function: see FIG. 25
[0198]In this embodiment, a favorable synthesized transfer function cannot be obtained no matter how long the fiber length of the interferometer 20 is. A wide flat mark region FWm will not be obtained.
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